NEW_Accomplishments.indd - IRIS
NEW_Accomplishments.indd - IRIS
NEW_Accomplishments.indd - IRIS
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2006 <strong>IRIS</strong> 5-YEAR PROPOSAL UPWELLING AND DOWNWELLING<br />
Seismic Evidence for Hotspot-Induced Buoyant Flow Beneath the<br />
Reykjanes Ridge<br />
James B. Gaherty • Lamont-Doherty Earth Observatory of Columbia University<br />
Volcanic hotspots and mid-ocean ridge spreading centers are the surface expressions of upwelling in Earthʼs mantle convection<br />
system, and their interaction provides unique information on upwelling dynamics. I investigated the influence of the<br />
Iceland hotspot on the adjacent mid-Atlantic spreading center (the Reykjanes Ridge, RR) using seismic surface waves from<br />
mid-Atlantic ridge earthquakes recorded at the Global Seismic Network station BORG and stations of the ICEMELT and<br />
HOTSPOT PASSCAL deployments (left). The surface waves from these events travel along and adjacent to the RR, and the<br />
travel times of these waves are sensitive to the average crust and upper-mantle velocity along each path. These delay times<br />
were inverted for age-dependent models of radial anisotropy (right). The models show a distinct pattern of shear anisotropy<br />
(∆V S ), with negative values (V SV > V SH ) above about 100 km depth, and positive values between about 100-200 km depth.<br />
This pattern of anisotropy is unlike that in comparable oceanic models, which display ∆V S > 0 throughout the upper 200 km<br />
of the mantle. This anisotropy suggests that the hotspot induces buoyancy-driven upwelling in the mantle beneath the ridge.<br />
In this model, the melt-zone upwelling is driven by buoyancy associated with retained melt, melt residuum, and/or locally hot<br />
(left) Bathymetric map of the North Atlantic study region. Surface waves of earthquakes (open circles) from the Reykjanes<br />
Ridge (RR) and the Gibbs Fracture Zone (GFZ) were recorded on Iceland at BORG and the ICEMELT and HOT-<br />
SPOT stations (inverted and upright triangles, respectively). Seafloor age is contoured at 20 Ma intervals. (right) Upper-mantle<br />
shear-velocity models of the Reykjanes region. Left panel displays mean shear speed (vS = (vSH+vSV)/2),<br />
while right panel displays shear anisotropy (vS = (vSH-vSV)/vS) in percent). Three age regions are shown: 0-5 Ma<br />
(short dash), 10-15 Ma (long dash), and 25-40 Ma (solid). Also shown (dash-dot lines) are shear-velocity models for<br />
Pacific upper-mantle (Nishimura and Forsyth, 1989).<br />
mantle. Such models produce a tight circulation within the melting zone, and as the mantle material moves out of the spreading<br />
center, a near-vertical fabric associated with the downgoing limb of the circulation is retained in the off-axis lithosphere<br />
to a depth of ~60-100 km. This result suggests that buoyancy-driven upwelling is an important component of ridge dynamics,<br />
especially in environments where passive sea-floor spreading is too slow to accommodate melt production. It also implies<br />
that the anisotropic structure of oceanic lithosphere may not be as simple as inferred through studies from the fast-spreading<br />
Pacific ridges, and that this structure holds important clues to ridge and plume dynamics.<br />
Gaherty, J.B., Seismic evidence for hotspot-induced buoyant flow beneath the Reykjanes Ridge, Science, 293, 1645-1647, 2001.<br />
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